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 /* NRDF D1809 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1809;
 TITLE=/Spectral measurements of neutrons, protons, deuterons and
        tritons produced by 100 MeV/nucleon He bombardment/;
 PURPOSE=/To present the angular-energy distributions of neutrons,
          protons, deuterons and tritons produced from thick carbon,
          aluminum, copper and lead targets bombarded by 100 MeV/nucleon
          helium ion. /;
 ATH=(T.KUROSAWA'1', T.NAKAMURA'1', N.NAKAO'2', T.SHIBATA'3',
      Y.UWAMINO'4', A.FUKUMURA'5');
 INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNKEK'3', 2JPNIPC'4', 2JPNIRS'5');
      /* '1' Cyclotron and Radioisotope Center */
      /* '2' Tanashi Branch */
 REF=NIM/A;
 VLP=430(1999)400;
 RCTS=(12C(ALPHA,P)X, 27AL(ALPHA,P)X, CU(ALPHA,P)X, PB(ALPHA,P)X,
       12C(ALPHA,D)X, 27AL(ALPHA,D)X, CU(ALPHA,D)X, PB(ALPHA,D)X,
       12C(ALPHA,T)X, 27AL(ALPHA,T)X, CU(ALPHA,T)X, PB(ALPHA,T)X);
 PHQS=ENGY-SPEC'6';
 /* '6' Double differential thick target yield */
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2003-09-13 : Compiled */
 PHQ=ENGY-SPEC'7';
 /* '7' Double differential thick target yield */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'8';
 /* '8' Heavy Ion Medical Accelerator in Chiba (HIMAC) */
 INST-ACC=2JPNIRS;
 INC-ENGY-LAB=100MEV/A;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'9',SCT'10',TOF'11',EDE'12');
 /* '9' Plastic scintillator (NE102A) was used as the delta-E
        counter, ToF start signal detector, and incident projectile
        counter */
 /* '10' Liquid scintillator (NE213) was used as the E counter */
 /* '11' To measure the energy of outgoing neutrons, protons,
         deuterons and tritons */
 /* '12' To eliminate charged particles */
 ANL=MONTE-MTHD'13';
 /* '13' LAHET Monte Carlo Code System, LCS [R.E. Prael, H.
         Lichtenstein, LA-UR-89-3014, Los Alamos National Laboratory,
         1989.] */
 /* Experimental Method:
    - Time-of-flight (To measure the energy of outgoing neutrons,
      protons, deuterons and tritons)
    - Particle identification by 'E/Delta E' measurement (To
      eliminate charged particles)
 RCT=12C(ALPHA,P)X;
 THK-TGT=8850MG/CM**2;
 DET-PARTCL=P;
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'20',<1%'21',<1%'22');
 /* '20' Uncertainty in the number of accepted beam particles
         incident on the target is estimated to be less than 3%. */
 /* '21' Uncertainty in the solid angle for the thickest carbon
         target, which has the maximum uncertainty, is less than 1%. */
 /* '22' Uncertainty of charged particle detection efficiency is
         estimated to be 1%, considering a small fraction of the slant
         incidence of a particle onto the detector. */
 STATIST-ERR=X%'23';
 /* '23' The statistical uncertainties vary from 2-5% in the low
         to medium energy (5-50 MeV) region of the spectra and increase
         to about 30% at the highest energies. */
 EMT=P;
 THTL=7.5DEG;
 DELTA-DN/DOMEGA/DE=<4%'24';
 /* '24' Total normalization uncertainty */
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-LAB-MIN'25' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'26'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   X         28.320   0.00027559
   28.320    31.370   0.0013878
   31.370    34.950   0.0016169
   34.950    38.685   0.0020089
   38.685    43.067   0.0020770
   43.067    48.259   0.0019929
   48.259    53.637   0.0022584
   53.637    59.998   0.0018814
   59.998    66.430   0.0020083
   66.430    73.999   0.0017817
   73.999    83.001   0.0011937
   83.001    91.885   0.0010873
   91.885    102.36   0.00074722
   102.36    114.85   0.00052710
   114.85    129.94   0.00024569
   129.94    144.44   0.00018307
   144.44    161.72   0.00011393
   161.72    182.63   5.4059e-05
   182.63    208.33   1.5875e-05
   208.33    231.79   7.9058e-06
   231.79    260.01   2.7938e-06
   260.01    294.53   8.0600e-07
 \END;
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